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Beam Diagnostics Using Synchrotron Radiation: Theory and Practice US Particle Accelerator School University of California, Santa Cruz San Francisco 2010 January 18 to 22 Pinhole Cameras Operation and Analysis Jeff Corbett a , Alan Fisher a , Walter Mok a , Weixing Cheng b a - SLAC National Accelerator Laboratory b - Brookhaven National Laboratory

Pinhole Cameras – Operation and Analysisuspas.fnal.gov/materials/10UCSC/Lecture_1d_Pinhole_Camera_2.pdfJan/18/2010 Pinhole Cameras –Operation and Analysis 10 2 2 2 2 image M source

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Page 1: Pinhole Cameras – Operation and Analysisuspas.fnal.gov/materials/10UCSC/Lecture_1d_Pinhole_Camera_2.pdfJan/18/2010 Pinhole Cameras –Operation and Analysis 10 2 2 2 2 image M source

Beam Diagnostics Using Synchrotron Radiation:

Theory and PracticeUS Particle Accelerator School

University of California, Santa Cruz

San Francisco — 2010 January 18 to 22

Pinhole Cameras – Operation and Analysis

Jeff Corbetta, Alan Fishera, Walter Moka, Weixing Chengb

a - SLAC National Accelerator Laboratoryb - Brookhaven National Laboratory

Page 2: Pinhole Cameras – Operation and Analysisuspas.fnal.gov/materials/10UCSC/Lecture_1d_Pinhole_Camera_2.pdfJan/18/2010 Pinhole Cameras –Operation and Analysis 10 2 2 2 2 image M source

• Low-emittance beam at 3rd generation light sources and HEP accelerators (ILC damping ring, superB, ERL, SLS /SOLEIL /Diamond /SSRF /ALBA /PETRA-III /NSLS2 etc…)

• Horizontal emittance ~ 1 nm.rad, vertical emittance ~ 10 pm.rad

• Typical beam size < 10um vertically (100um horizontal)

• Q: How to measure such a small beam?– Visible light image of synchrotron radiation (diffraction > 50um)

– Wire scan, laser wire (minutes for a full scan, 1-D)

– Interferometer (~10um resolution)

– Vertical beam size from p-mode radiation

– X-ray pinhole (simple, ~5um resolution)

– Fresnel zone plate (x-ray imaging of monochromatic beam, used at ATF, Spring-8 etc.)

– X-ray refractive optics (monochromatic light, complicated)

Small beams need to be measured

Jan/18/2010 2Pinhole Cameras – Operation and Analysis

Page 3: Pinhole Cameras – Operation and Analysisuspas.fnal.gov/materials/10UCSC/Lecture_1d_Pinhole_Camera_2.pdfJan/18/2010 Pinhole Cameras –Operation and Analysis 10 2 2 2 2 image M source

First Observation of Pinhole Image

Jan/18/2010 3Pinhole Cameras – Operation and Analysis

“景到(倒),在午有端,与景长,说在端” 《墨经》

The image is upside down, because of the pinhole in the wall.

墨子 (468-376 B.C.)

Page 4: Pinhole Cameras – Operation and Analysisuspas.fnal.gov/materials/10UCSC/Lecture_1d_Pinhole_Camera_2.pdfJan/18/2010 Pinhole Cameras –Operation and Analysis 10 2 2 2 2 image M source

Camera Obscura

Jan/18/2010 4Pinhole Cameras – Operation and Analysis

object

imagepinhole

d1 d2

1

2d

dM

Page 5: Pinhole Cameras – Operation and Analysisuspas.fnal.gov/materials/10UCSC/Lecture_1d_Pinhole_Camera_2.pdfJan/18/2010 Pinhole Cameras –Operation and Analysis 10 2 2 2 2 image M source

X-ray Pinhole Camera - Schematic

Jan/18/2010 5Pinhole Cameras – Operation and Analysis

SPEAR

Soleil

Page 6: Pinhole Cameras – Operation and Analysisuspas.fnal.gov/materials/10UCSC/Lecture_1d_Pinhole_Camera_2.pdfJan/18/2010 Pinhole Cameras –Operation and Analysis 10 2 2 2 2 image M source

SPEAR3 Pinhole, Filters, YAG Screen and Camera

Jan/18/2010 6Pinhole Cameras – Operation and Analysis

Page 7: Pinhole Cameras – Operation and Analysisuspas.fnal.gov/materials/10UCSC/Lecture_1d_Pinhole_Camera_2.pdfJan/18/2010 Pinhole Cameras –Operation and Analysis 10 2 2 2 2 image M source

SPEAR3 pinhole results

Jan/18/2010 7Pinhole Cameras – Operation and Analysis

x-position [mm] x-position [mm]in

tensity [

au]

inte

nsity [

au]

Measurement Theory

Three optics available:

– Low emittance

– Achromatic

– Low-alpha

22

E

Exxx

yyy 2

Page 8: Pinhole Cameras – Operation and Analysisuspas.fnal.gov/materials/10UCSC/Lecture_1d_Pinhole_Camera_2.pdfJan/18/2010 Pinhole Cameras –Operation and Analysis 10 2 2 2 2 image M source

BESSY-II Pinhole Array

Jan/18/2010 8Pinhole Cameras – Operation and Analysis

Constant Image Intensity

Fin

ite

be

am

div

erg

en

ce

Used at ALS and ASP as well

Beam size & divergence

Page 9: Pinhole Cameras – Operation and Analysisuspas.fnal.gov/materials/10UCSC/Lecture_1d_Pinhole_Camera_2.pdfJan/18/2010 Pinhole Cameras –Operation and Analysis 10 2 2 2 2 image M source

Optimize the pinhole size

Jan/18/2010 9Pinhole Cameras – Operation and Analysis

If the pinhole is large, ray-optic „spread‟ dominates

d1 d2

w

1

)21

(

d

ddw

If the pinhole is small, diffraction dominates...

Geometric error

Diffraction error

Other measurement errors include: Screen, CCD camera and

chromatic error etc

Page 10: Pinhole Cameras – Operation and Analysisuspas.fnal.gov/materials/10UCSC/Lecture_1d_Pinhole_Camera_2.pdfJan/18/2010 Pinhole Cameras –Operation and Analysis 10 2 2 2 2 image M source

Optimize the pinhole size (cont’)

Jan/18/2010 10Pinhole Cameras – Operation and Analysis

2222

ndiffractioblursourceimage M

1

21

2 L

LLwblur

p

w

Lndiffractio

2

4

12

p

L1 Distance from source point to pinhole

L2 Distance from pinhole to screen

M=L2/L1, magnification factor

W pinhole size

~ 40 mm

Page 11: Pinhole Cameras – Operation and Analysisuspas.fnal.gov/materials/10UCSC/Lecture_1d_Pinhole_Camera_2.pdfJan/18/2010 Pinhole Cameras –Operation and Analysis 10 2 2 2 2 image M source

Optimize the pinhole size (cont’)

Jan/18/2010 11Pinhole Cameras – Operation and Analysis

Geometric error:

Diffraction error:

SRW PSF simulationa – pinhole width

d – distance from source point to pinhole

D – distance from pinhole to screen

E – photon energy in eV unit

Different curve corresponding to different filters

Page 12: Pinhole Cameras – Operation and Analysisuspas.fnal.gov/materials/10UCSC/Lecture_1d_Pinhole_Camera_2.pdfJan/18/2010 Pinhole Cameras –Operation and Analysis 10 2 2 2 2 image M source

‘Polychromatic’ Diffraction

Jan/18/2010 12Pinhole Cameras – Operation and Analysis

Integrate intensity pattern over photon spectrum

spectrum at screen

dN/dE: Photons/sec/keV

Sands-121

C. Limborg - SSRL

Page 13: Pinhole Cameras – Operation and Analysisuspas.fnal.gov/materials/10UCSC/Lecture_1d_Pinhole_Camera_2.pdfJan/18/2010 Pinhole Cameras –Operation and Analysis 10 2 2 2 2 image M source

PSF Calculation

Jan/18/2010 13Pinhole Cameras – Operation and Analysis

Ay=40 micron

(optimum)

Ay=5 micron

(diffraction)Ay=250 micron

(geometric)

143mm 250mm78mm

J. Bergstrom - CLS

Putting it all together…

fresnel.m valid from geometric to diffraction regimes

SRW, SPECTRA etc. can do the similar job

Page 14: Pinhole Cameras – Operation and Analysisuspas.fnal.gov/materials/10UCSC/Lecture_1d_Pinhole_Camera_2.pdfJan/18/2010 Pinhole Cameras –Operation and Analysis 10 2 2 2 2 image M source

Phosphor screen error

Jan/18/2010 14Pinhole Cameras – Operation and Analysis

Diamond, screens compare

Power phosphor screen YAG

To select the screen:

– Spatial resolution

– Time response (decay time,

70ns for YAG:Ce)

– Photon yield of the screen

– Emission wavelength

– Radiation damage etc.

Page 15: Pinhole Cameras – Operation and Analysisuspas.fnal.gov/materials/10UCSC/Lecture_1d_Pinhole_Camera_2.pdfJan/18/2010 Pinhole Cameras –Operation and Analysis 10 2 2 2 2 image M source

CCD error

Jan/18/2010 15Pinhole Cameras – Operation and Analysis

CCD – Charge Coupled Device

Finite pixel size (Flea2, 4.65 x 4.65µm pixel size)

Spilling to neighbors due to spilled charge or scattered radiation

][,_3.0 pixelsfractionspillccd Screen and CCD errors are negligible if the pinhole magnification

factor is large

Page 16: Pinhole Cameras – Operation and Analysisuspas.fnal.gov/materials/10UCSC/Lecture_1d_Pinhole_Camera_2.pdfJan/18/2010 Pinhole Cameras –Operation and Analysis 10 2 2 2 2 image M source

Summary

Jan/18/2010 16Pinhole Cameras – Operation and Analysis

- Pinhole cameras effective in the x-ray regime (~5mm resolution)

- System construction fairly straight-forward

- Power loading considerations

- Optimize aperture size

- Data analysis relies on comparison of model with measurement

fresnel.m

- Relative high exposure time due to small aperture (fast measurement

needed for injection transient and machine physics)